Capacitor that includes high permittivity capacitor dielectric

ABSTRACT

A decoupling capacitor is formed on a semiconductor substrate that includes a silicon surface layer. A substantially flat bottom electrode is formed in a portion of the semiconductor surface layer. A capacitor dielectric overlies the bottom electrode. The capacitor dielectric is formed from a high permittivity dielectric with a relative permittivity, preferably greater than about 5. The capacitor also includes a substantially flat top electrode that overlies the capacitor dielectric. In the preferred application, the top electrode is connected to a first reference voltage line and the bottom electrode is connected to a second reference voltage line.

This application is a divisional of patent application Ser. No. 11/167,694, entitled “Capacitor that Includes High Permittivity Capacitor Dielectric,” filed on Jun. 27, 2005, now U.S. Pat. No. 7,037,772, which is a divisional of patent application Ser. No. 10/628,020, entitled “Capacitor that Includes High Permittivity Capacitor Dielectric,” filed on Jul. 25, 2003, now U.S. Pat. No. 6,936,881, which applications are incorporated herein by reference.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application relates to the following co-pending and commonly assigned patent application Ser. No. 10/627,218, filed Jul. 25, 2003 and entitled “Capacitor with Enhanced Performance and Method of Manufacture,” which application is hereby incorporated herein by reference.

TECHNICAL FIELD

The present invention relates generally to semiconductor devices and more particularly to a capacitor with enhanced performance and method of manufacture.

BACKGROUND

Power supply lines in a semiconductor integrated circuit chip supply current to charge and discharge active and passive devices in the integrated circuit. For example, digital complementary metal-oxide-semiconductor (CMOS) circuits draw current when the clock makes a transition. During the operation of circuits, the power supply lines must supply transient currents with a relatively high intensity, and can result in voltage noise on the power supply lines. The voltage on the power supply line will fluctuate when the fluctuation time of the transient current is short or when its parasitic inductance or parasitic resistance is large.

In state-of-the-art circuits, the operational frequency of the integrated circuit is in the order of several hundreds of mega-hertz (MHz) to several giga-hertz (GHz). In such circuits, the rising time of clock signals is very short, so that voltage fluctuations in the supply line can be very large. Undesired voltage fluctuations in the power supply line powering a circuit can cause noise on its internal signals and degrade noise margins. The degradation of noise margins can reduce circuit reliability or even cause circuit malfunction.

To reduce the magnitude of voltage fluctuations in the power supply lines, filtering or decoupling capacitors are usually used between the terminals of different power supply lines or between terminals of power supply line and the ground line. Decoupling capacitors act as charge reservoirs that additionally supply currents to circuits when required to prevent momentary drops in supply voltage.

FIG. 1 shows a circuit diagram containing these decoupling capacitors. Capacitor C₁ is a decoupling capacitor that is inserted between a power supply line V_(DD) and the ground line GND. Most chips employ more than one power supply line, and may have a different power supply line OV_(DD) for the output circuits that interface with external circuits. Capacitor C₂ is a decoupling capacitor that is inserted between the output voltage supply line OV_(DD) and the ground line GND. Capacitor C₃ is a decoupling capacitor that is inserted between the supply line V_(DD) and the output voltage supply line OV_(DD). These decoupling capacitors are usually placed as close as possible to the transient current source or sink.

Decoupling capacitors are used in integrated chips employing both bulk and silicon-on-insulator substrates. However, the role of decoupling capacitors is more important in a silicon-on-insulator chip than in a bulk silicon chip due to the following reason. Integrated chips fabricated on bulk substrates can naturally decouple the power supply potential and the ground potential due to the presence of inherent depletion capacitances between the doped wells and the bulk substrate. Compared to bulk substrates, silicon-on-insulator chips have very low on-chip decoupling capacitance between the power supply lines and ground.

U.S. Pat. No. 6,558,998 entitled “SOI type integrated circuit with a decoupling capacity and process for embodiment of such a circuit” issued to Belleville et al. describes a decoupling capacitor that is formed with the formation of silicon-on-insulator substrates. While that capacitor may be formed with a large area or large capacitance, it is formed together with the substrate, which means that the substrate has to be customized for each different circuit design.

SUMMARY OF THE INVENTION

These and other problems are generally solved or circumvented, and technical advantages are generally achieved, by preferred embodiments of the present invention which teach an integrated circuit capacitor with improved capacitance density and method of manufacture a capacitor.

In accordance with a preferred embodiment of the present invention, a capacitor is formed in a capacitor includes an insulating layer overlying a substrate. A semiconductor layer overlies the insulator layer and a bottom electrode is formed in a portion of the semiconductor layer. A capacitor dielectric overlies the bottom electrode. Preferably, the capacitor dielectric comprising a high permittivity dielectric having a dielectric constant greater than about 5. A top electrode overlies the capacitor dielectric.

The preferred embodiment provides a decoupling capacitor that is formed on a semiconductor substrate that includes a silicon surface layer. A substantially flat bottom electrode is formed in a portion of the semiconductor surface layer. A capacitor dielectric overlies the bottom electrode and has a relative permittivity greater than about 5. A substantially flat top electrode overlies the capacitor dielectric. The top electrode is connected to a first reference voltage line and the bottom electrode is connected to a second reference voltage line.

The foregoing has outlined rather broadly the features and technical advantages of the present invention in order that the detailed description of the invention that follows may be better understood. Additional features and advantages of the invention will be described hereinafter which form the subject of the claims of the invention. It should be appreciated by those skilled in the art that the conception and specific embodiment disclosed may be readily utilized as a basis for modifying or designing other structures or processes for carrying out the same purposes of the present invention. It should also be realized by those skilled in the art that such equivalent constructions do not depart from the spirit and scope of the invention as set forth in the appended claims.

BRIEF DESCRIPTION OF THE DRAWINGS

For a more complete understanding of the present invention, and the advantages thereof, reference is now made to the following descriptions taken in conjunction with the accompanying drawing, in which:

FIG. 1 shows an equivalent circuit of known decoupling capacitors;

FIG. 2 provides a cross-sectional view of a preferred embodiment of this invention;

FIG. 3 is a top view or layout view of a capacitor of the preferred embodiment;

FIGS. 4 a and 4 b show cross-sectional views of a capacitor of a preferred embodiment;

FIGS. 5 a and 5 b show other cross-sectional views of a capacitor of a preferred embodiment; and

FIGS. 6 a-6 f show cross-sectional views of a capacitor of the preferred embodiment during various stages of the fabrication process.

DETAILED DESCRIPTION OF ILLUSTRATIVE EMBODIMENTS

The making and using of the presently preferred embodiments are discussed in detail below. It should be appreciated, however, that the present invention provides many applicable inventive concepts that can be embodied in a wide variety of specific contexts. The specific embodiments discussed are merely illustrative of specific ways to make and use the invention, and do not limit the scope of the invention.

In the preferred embodiment this invention, a capacitor structure with a high permittivity dielectric is formed on a silicon-on-insulator substrate. The following discussion provides further details on the various embodiments and methods of manufacture.

The preferred embodiment of the present invention relates to a capacitor, and more specifically, to capacitors formed with improved capacitance density. As an example, these capacitors can be used as decoupling capacitors. A number of examples and methods of fabrication will be discussed below.

In the preferred embodiment of this invention, capacitors with improved capacitance density are taught. Such capacitors are useful as decoupling capacitors that help reduce voltage fluctuations in voltage supply lines in integrated circuit chips. The decoupling capacitors taught in this invention can be used on bulk substrates comprising an elemental semiconductor such as silicon, bulk substrates comprising of an alloy semiconductor such as silicon-germanium, or bulk substrates comprising of a compound semiconductor such as indium phosphide. More preferably, the decoupling capacitors may be formed on semiconductor-on-insulator substrates such as silicon-on-insulator substrates.

FIG. 2 provides a cross-sectional view of a preferred embodiment of this invention. In this embodiment, a decoupling capacitor 102 is formed on a semiconductor-on-insulator substrate that includes a semiconductor layer 104 on an insulator layer 106, which in turn overlies a substrate 108, preferably a silicon substrate. The capacitor 102 includes a bottom electrode 110, a capacitor dielectric 112 overlying the bottom electrode 110, and a top electrode 114 overlying the capacitor dielectric 112.

The bottom electrode 110 is preferably formed within the semiconductor layer 104. The bottom electrode 110 may be lightly-doped and electrically contacted by a highly-doped region (not shown in FIG. 2, see e.g., FIG. 4 b). Alternatively, the bottom electrode 110 may be a highly-doped region. In various embodiments, the bottom electrode may be doped with n-type (e.g., arsenic or phosphorus) or p-type (e.g., boron) dopants.

The capacitor dielectric 112 is preferably a high permittivity (high-k) dielectric. By using a high-k dielectric as the capacitor dielectric 112, the capacitance density

$\frac{ɛ_{0}ɛ_{r}}{t_{phys}}$ is significantly higher than that of a capacitor employing a conventional silicon oxide dielectric, where ε₀ is the permittivity of free space, ε_(r) is the relative permittivity, and t_(phys) is the physical thickness of the capacitor dielectric. If the decoupling capacitor 102 maintains the same size (i.e., length×width of bottom and top electrodes 110 and 112), the use of a high-k capacitor dielectric improves the total capacitance and therefore reduces the voltage fluctuations in the voltage supply lines to which it decouples.

The high-k dielectric preferably has a relative permittivity of larger than 5, and more preferably has a relative permittivity of larger than 10, and even more preferably has a relative permittivity of larger than 20. The high permittivity dielectric may be selected from a group comprising of aluminum oxide (Al₂O₃), hafnium oxide (HfO₂), haffiium oxynitride (HfON), hafnium silicate (HfSiO₄), zirconium oxide (ZrO₂), zirconium oxynitride (ZrON), zirconium silicate (ZrSiO₄), or combinations thereof. In the preferred embodiment, the high-k dielectric is hafnium oxide.

The silicon oxide equivalent thickness (EOT) of the capacitor dielectric 112 is preferably smaller than about 100 angstroms, more preferably smaller than about 50 angstroms, and even more preferably smaller than about 10 angstroms. The physical thickness of the capacitor dielectric may be smaller than about 100 angstroms, more preferably smaller than about 50 angstroms, and even more preferably smaller than about 10 angstroms. In other embodiments, the physical thickness of the capacitor dielectric may be smaller than about 100 angstroms, more preferably smaller than about 50 angstroms, and even more preferably smaller than about 10 angstroms.

The top electrode 114 is formed from a conductive material such as poly-crystalline silicon, poly-crystalline silicon-germanium, a metal, a metallic nitride, a metallic silicide, or a metallic oxide, or combinations thereof. Metals such as molybdenum, tungsten, titanium, tantalum, platinum, and hafnium may be used as the portion of the top electrode. Metallic nitrides may include, but will not be restricted to, molybdenum nitride, tungsten nitride, titanium nitride, tantalum nitride. Metallic silicides may include, but will not be restricted to, nickel silicide, cobalt silicide, tungsten silicide, titanium silicide, tantalum silicide, platinum silicide, erbium silicide. Metallic oxides may include, but will not be restricted to, ruthenium oxide and indium tin oxide.

As shown in FIG. 2, the decoupling capacitor may be formed in an active region in the vicinity of an active device such as a transistor 116. The transistor 116 includes source and drain regions 118 and 120 in silicon layer 104, a gate dielectric 122, and a gate electrode 124. In the preferred embodiment, the gate dielectric 122 is formed from the same layer as the capacitor dielectric 112 and the gate electrode 124 is formed from the same layer as the top electrode 114. In fact, as will be discussed below, the transistor 116 and capacitor 102 are preferably formed at the same time.

FIG. 2 also illustrates a third active region 126. While no device is shown in active region 126, it is understood that a capacitor, a transistor or another device such as a diode or a resistor can be formed. In fact a typical semiconductor chip will include many different device components formed. In some cases, a number of devices will be formed in a single active region while in other cases a single active region will include only one element.

Active region 126 is isolated from the active region that includes capacitor 102 and the active region that includes transistor 116 by isolation regions 128. In the illustrated embodiment, shallow trench isolation (STI) is used. In this case, an insulator, such as silicon oxide, is formed within a trench between active areas. In the preferred embodiment, the STI dielectric fill material is chemical vapor deposited silicon oxide. The shallow trench isolation structure may also comprise trench liner oxide (not shown for simplicity) on the boundaries of the trench. The trench liner oxide may or may not contain nitrogen. In other embodiments, other isolation techniques such as mesa isolation can be used. In those cases, the trenches are left unfilled during formation of the devices in the active regions.

FIG. 3 is a top view or layout view of the capacitor 102 of the preferred embodiment. The capacitor 102 has a width W and a length L. In the preferred embodiment, the width W may have a dimension of greater than about 5 microns, and preferably greater than about 10 microns. In the preferred embodiment, the length L may have a dimension of greater than about 1 micron, and preferably greater than about 5 microns. The detailed structure of the capacitor may be seen in cross-sectional views along the lines A-A′ and B-B′, which are shown in FIGS. 4 a and 4 b. The contacts 130 are shown in the cross-sectional views of FIGS. 5 a and 5 b, for example.

The cross-sectional view along line A-A′ is shown in FIG. 4 a. The top electrode 114 extends laterally over the isolation regions 128. The top electrode in FIG. 4 a is shown to have a thickness t, preferably in the range of about 200 angstroms to about 2000 angstroms. The capacitor structure 102 may additionally have spacers 132 formed on the sides of the top electrode 114. In a typical embodiment, these spacers 132 are formed during formation of transistor 116 (FIG. 2) and therefore also included with the capacitor 102. The spacers 132, however, are optional.

The cross-sectional view along line B-B′ is shown in FIG. 4 b. FIG. 4 b shows that the bottom electrode 110 can be electrically connected via adjacent doped regions 134 and 136. One or more doped regions 134 (136) can be included. In the case where the bottom electrode 110 is not heavily doped, the bottom electrode 110 may include an inversion layer. An inversion layer may be formed by a supply of mobile carriers from the adjacent doped regions, and when there is a substantial bias between the top and bottom electrodes 110 and 114. The substantial bias can be the potential between V_(DD) and GND, between OV_(DD) and GND, or between OV_(DD) and V_(DD).

In one embodiment, the bottom electrode 110 is doped to the same conductivity type as the contact regions 134 and 136. That is, the impurities added to the silicon layer 104 are the same conductivity type (n or p) for bottom electrode 110 and contact regions 134 and 136.

In another embodiment, the bottom electrode 110 is doped to a different conductivity type. In this case, the inversion region creates the contact between regions 110, 134 and 136. For example, in one embodiment the contact regions 134 and 136 are physically doped with n-type dopants (e.g., arsenic and/or phosphorus) and the electrode region 110 is physically doped with p-type dopants (e.g., boron). When the top electrode 114 is connected to a high enough voltage level, an inversion region will be formed in bottom electrode 110, which will appear to be n-doped. In this manner, the bottom electrode contact regions 134 and/or 136 are doped to a given conductivity type (n-type in this example) and the bottom electrode 110 is operationally doped the given conductivity type. In this context, “operationally doped” means being at that doping level whenever the chip is operational. This definition excludes a transistor, which is at that doping level only when that transistor itself, rather than the chip, is turned on.

An embodiment showing the contacts 130 and 131 to the bottom and top electrodes 110 and 114 is shown in FIGS. 5 a and 5 b (collectively FIG. 5). FIG. 5 a shows a cross-sectional view along line A-A′ of FIG. 3 and FIG. 5 b shows a cross-sectional view along line B-B′ of FIG. 3.

The views of FIG. 5 include an inter-layer dielectric 138. The inter-layer dielectric (ILD) 138 can be a chemical vapor deposited dielectric such as silicon oxide. The ILD 138 can also be a low permittivity (low-k) dielectric employed in interconnect technology. By using a low-k ILD to cover the capacitor 102, parasitic capacitances between the top electrode 114 and metal lines 140 in the vicinity of the top electrode 114 can be reduced.

In the preferred embodiment, the relative-permittivity of the low-k dielectric 138 is less than about 3.5, and more preferably less than about 3.0. For example, the low-k dielectric material can be an organic material, such as benzocyclobutene (BCB), SILK, FLARE, or others. Alternatively, the low-k dielectric material can be an inorganic dielectric material, such as methyl silsesquioxane (MSQ), hydrogen silsesquioxane (HSQ), SiOF, for example. These materials are exemplary only as other embodiments may include different low-k dielectric materials.

A contact etch-stop layer 144 can overlie the top electrode 114 and the spacer 132, as shown in FIG. 5. The contact etch-stop layer 144 is preferably silicon nitride, but it is understood that other materials with a different etch rate from the ILD 138 can be used. The silicon nitride etch-stop layer 144 can have an inherent stress in the range of −2 giga-pascals (GPa) to +2 GPa, where negative stress implies compressive stress and positive stress implies tensile stress.

A contact plug 131 electrically couples the top electrode 114 to interconnect metal lines 140 as shown in FIG. 5 a. As shown in FIG. 5 b, a contact plug 130 electrically couples the doped region 134 (135) in the semiconductor layer 104 with the bottom electrode 110. The contact plugs are made of a conductive material such as tungsten and may include barrier layers (not shown), e.g., titanium and titanium nitride.

A inter-metal dielectric (IMD) 142 is formed over metal layer 140 and ILD 138. The IMD 142 can be formed from any of the materials listed above. The IMD 142 can be the same material or a different material than ILD 138. While not shown, contacts can be formed through the IMD 142 to contact metal layer 140.

It is understood that the capacitor 102 can be used in a semiconductor-on-insulator technology employing trench isolation, or may be used in a semiconductor-on-insulator technology employing mesa isolation. In mesa isolation, trenches are not filled with a dielectric filling material prior to the formation of transistors or capacitors. In a semiconductor chip employing mesa isolation, trenches between active regions are not filled with dielectric prior to the formation of active devices.

Next, a method of manufacturing a capacitor will be described with respect to FIGS. 6 a-6 f. As will be discussed, the capacitor can be formed at the same time as a transistor (see e.g., transistor 116 in FIG. 2).

Referring now to FIG. 6 a, a semiconductor-on-insulator substrate including substrate 108, insulator 106 and semiconductor layer 104 is provided. An active region mask 148 is used to define trenches 150 in the semiconductor layer 104. The semiconductor layer 104 preferably has a thickness of about 1000 angstroms or thinner. The insulator 106 thickness is preferably about 1200 angstroms or thinner. The mask 148 preferably comprises silicon nitride, and more preferably comprises silicon nitride on a silicon oxide layer.

Trench filling dielectric material is deposited by chemical vapor deposition to fill the trenches 150, followed by a chemical mechanical planarization process step. The mask 148 is then removed to give the cross-section as shown in FIG. 6 b. The bottom electrode 110 may or may not be heavily doped at this point. If an ion implantation step with a high dose is introduced into the active region at this point to dope the semiconductor layer 104, a heavily-doped bottom electrode 110 can be formed. For example, the heavily-doped active region or bottom electrode 110 may have a doping concentration of greater than about 10¹⁹cm⁻³.

The capacitor dielectric 112 is then formed, as shown in FIG. 6 c. The physical thickness of the dielectric 112 may be larger than 5 angstroms, more preferably larger than 20 angstroms, and even more preferably larger than 40 angstroms. The capacitor dielectric 112 may be formed together with the formation of a transistor gate dielectric in a different portion of the semiconductor chip (not shown here, see FIG. 2). By forming the high-k capacitor dielectric together with the gate dielectric of a transistor in a different portion of the chip, no additional process steps are introduced.

High-k dielectric materials as previously described may be used. The high-k dielectric may be formed by chemical vapor deposition, sputter deposition, or other known techniques of forming high-k dielectric materials. An interfacial layer (not shown) can be formed on the bottom electrode 110 prior to the formation of the high-k dielectric material 112. The interfacial layer may be a silicon oxide layer or a silicon oxynitride layer. The active region may additionally be treated in a hydrogen-containing or nitrogen-containing ambient prior to the formation of the interfacial layer.

The top electrode 114 material can then be deposited over the capacitor dielectric layer 112. The top electrode material can be comprised of conventional poly-crystalline silicon, poly-crystalline silicon germanium, metals, metallic silicides, or metallic nitrides, as previously described. The top electrode material may be deposited by conventional techniques such as chemical vapor deposition. The top electrode may also be formed by the deposition of silicon and metal, followed by an anneal to form a metal silicide gate electrode material. The top electrode material is then patterned using photolithography techniques, and etched using plasma etch processes to form the gate electrodes.

The deposition of the top electrode 114 material may be the same process step as the deposition of gate electrode material of a transistor to be formed in a different portion of the semiconductor chip, and the etching of the top electrode may similarly be accomplished together with the etching of the gate electrode of the transistor. The completed top electrode 114 is shown in FIG. 6 d. The capacitor dielectric 112 is retained at least in the portion of the capacitor covered by the top electrode 114.

Doping may be introduced in regions adjacent to the bottom electrode to make electrical contacts with the bottom electrode 110. The electrical contact regions 134 and 136 are shown in the cross-sectional views of FIG. 4 b and FIG. 5 b (and are above and below the plane of the page in the view of FIG. 6 d. The doping of contact regions 134 and 136 is formed at the same time that source and drain regions of the transistor (116 in FIG. 2) are doped. For example, the doping step performed in FIG. 6 d can form the lightly doped extensions of the source and drain.

As shown in FIG. 6 e, spacers 132 may be additionally formed on the sides of the top electrode 114. This may be followed by another implant to doped the regions (134 and 136 in FIG. 4 b) of the active region not covered by the top electrode 114 and spacers 132. This step will simultaneously form the heavily doped source and drain regions of transistors on the chip.

A contact etch-stop layer 144 can be formed on the top electrode 114 and spacers 132. An inter-layer dielectric (ILD) 142 can be formed over the capacitor and contact holes 131 (and 130 in FIG. 5 b) can be etched through the ILD 142 to reach the top and bottom electrodes 110 and 114. Conductive materials, such as tungsten, are then used to fill the contact holes to electrically contact the top and bottom electrodes to metal layers (see e.g., metal layer 140 in FIG. 5 b).

Although the capacitor described in this invention has been illustrated for use as a decoupling capacitance, it is understood that the capacitor thus formed according to this invention may be used for other purposes. For example, the capacitor may be used as a coupling capacitor.

In the foregoing specification, the invention has been described with reference to specific embodiments. However, various modifications and changes can be made by one skilled in the art without departing from the scope of the present invention. Accordingly, the specification and figures are to be regarded in an illustrative rather than a restrictive sense, and all such modifications are intended to be included within the scope of the present invention.

While this invention has been described with reference to illustrative embodiments, this description is not intended to be construed in a limiting sense. Various modifications and combinations of the illustrative embodiments, as well as other embodiments of the invention, will be apparent to persons skilled in the art upon reference to the description. It is therefore intended that the appended claims encompass any such modifications or embodiments. 

1. A method of forming a decoupling capacitor, the method comprising: providing a semiconductor substrate that includes a silicon surface layer; forming a substantially flat bottom electrode in a portion of the silicon surface layer, the bottom electrode being doped to a first conductivity type; pre-treating the bottom electrode with a non-metal gas prior to forming an interfacial layer between the bottom electrode and a high permittivity capacitor dielectric; forming the interfacial layer over the pre-treated surface of the bottom electrode; simultaneously forming the high permittivity capacitor dielectric and a gate dielectric from a high permittivity dielectric with a relative permittivity greater than about 5, the high permittivity capacitor dielectric formed over the interfacial layer; forming a substantially flat top electrode over the high permittivity capacitor dielectric; forming a doped region within the silicon surface layer adjacent to the bottom electrode, the doped region doped to a second conductivity type; electrically coupling the top electrode to a first reference voltage line; and electrically coupling the bottom electrode to a second reference voltage line.
 2. The method of claim 1, wherein the non-metal gas is comprised of hydrogen.
 3. The method of claim 1, wherein the non-metal gas is comprised of nitrogen.
 4. The method of claim 1, wherein the interfacial layer is comprised of silicon oxide.
 5. The method of claim 1, wherein the interfacial layer is comprised of silicon oxynitride.
 6. The method of claim 1, wherein the bottom electrode is doped to a concentration greater than or equal to 1E19 cm⁻³. 